US9008741B2 - Superconducting structure comprising coated conductor tapes, in particular stapled perpendicularly to their substrate planes - Google Patents
Superconducting structure comprising coated conductor tapes, in particular stapled perpendicularly to their substrate planes Download PDFInfo
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- US9008741B2 US9008741B2 US13/760,110 US201313760110A US9008741B2 US 9008741 B2 US9008741 B2 US 9008741B2 US 201313760110 A US201313760110 A US 201313760110A US 9008741 B2 US9008741 B2 US 9008741B2
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- 239000004020 conductor Substances 0.000 title claims abstract description 318
- 239000000758 substrate Substances 0.000 title claims abstract description 55
- 229910021521 yttrium barium copper oxide Inorganic materials 0.000 claims abstract description 9
- 238000012546 transfer Methods 0.000 claims description 31
- 229910000679 solder Inorganic materials 0.000 claims description 22
- 229910000510 noble metal Inorganic materials 0.000 claims description 21
- 125000006850 spacer group Chemical group 0.000 claims description 19
- 239000002826 coolant Substances 0.000 claims description 14
- 229910045601 alloy Inorganic materials 0.000 claims description 10
- 239000000956 alloy Substances 0.000 claims description 10
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 claims description 7
- 229910052802 copper Inorganic materials 0.000 claims description 7
- 239000010949 copper Substances 0.000 claims description 7
- 229910052751 metal Inorganic materials 0.000 claims description 7
- 239000002184 metal Substances 0.000 claims description 7
- 239000003989 dielectric material Substances 0.000 claims description 5
- 239000002887 superconductor Substances 0.000 claims description 5
- 208000026817 47,XYY syndrome Diseases 0.000 description 12
- 239000000463 material Substances 0.000 description 12
- 230000007547 defect Effects 0.000 description 6
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- 239000004332 silver Substances 0.000 description 3
- 241000264877 Hippospongia communis Species 0.000 description 2
- ATJFFYVFTNAWJD-UHFFFAOYSA-N Tin Chemical compound [Sn] ATJFFYVFTNAWJD-UHFFFAOYSA-N 0.000 description 2
- 239000011248 coating agent Substances 0.000 description 2
- 238000000576 coating method Methods 0.000 description 2
- 239000007789 gas Substances 0.000 description 2
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 2
- 229910052737 gold Inorganic materials 0.000 description 2
- 239000010931 gold Substances 0.000 description 2
- 239000001307 helium Substances 0.000 description 2
- 229910052734 helium Inorganic materials 0.000 description 2
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 239000004593 Epoxy Substances 0.000 description 1
- BTGZYWWSOPEHMM-UHFFFAOYSA-N [O].[Cu].[Y].[Ba] Chemical compound [O].[Cu].[Y].[Ba] BTGZYWWSOPEHMM-UHFFFAOYSA-N 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
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Images
Classifications
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N60/00—Superconducting devices
- H10N60/20—Permanent superconducting devices
- H10N60/203—Permanent superconducting devices comprising high-Tc ceramic materials
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01B—CABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
- H01B12/00—Superconductive or hyperconductive conductors, cables, or transmission lines
- H01B12/02—Superconductive or hyperconductive conductors, cables, or transmission lines characterised by their form
-
- H01L39/08—
-
- H01L39/143—
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N60/00—Superconducting devices
- H10N60/80—Constructional details
- H10N60/83—Element shape
Definitions
- the invention relates to a superconducting structure comprising a plurality of coated conductor tapes, each with a substrate which is one-sided coated with a superconducting film, in particular an YBCO film,
- the superconducting structure provides a superconducting current path along an extension direction (z) of the superconducting structure
- coated conductor tapes provide electrically parallel partial superconducting current paths in the extension direction (z) of the superconducting structure.
- Superconductors are used to carry electric currents, typically with a high current strength, and may be included in different applications, such as current transfer lines or magnetic coils.
- Superconductors may, at a temperature below the so called critical temperature Tc, carry the electric current at practically no ohmic losses.
- the conductor is typically cooled, for example with liquefied gases such as liquid helium. Further, to have a superconducting state, it is also necessary to stay below a critical current density and below a critical magnetic field with the conductor.
- HTS high temperature superconductor
- YBCO yttrium barium copper oxide
- the superconducting film deposited on a substrate tape is relatively thin, and limits the absolute current strength that may be transported through the coated conductor. In order to increase the absolute current strength that may be transported, it is known to electrically connect a plurality of coated conductor tapes in parallel.
- HTS current lead device for connecting a superconducting current consumer with a current supply point, with the device comprising several HTS tapes arranged on a support in parallel and spaced apart from each other. Note that this structure is rather large scaled, and the support makes the structure unflexible.
- U.S. Pat. No. 7,774,035 B2 discloses superconducting articles wherein two superconductor tapes are bonded together, with the superconducting films facing away from each other.
- a coated conductor may easily be overloaded and lose its superconducting state (“quench”), what in turn often leads to a quench of the complete superconducting structure. Furthermore, the critical or quench current threshold is not sufficient.
- the total electric current is spread between the coated conductor tapes at their ends, and the current distribution is thus fixed over the length of the tapes.
- the current distribution between the coated conductor tapes may change along the extension direction, since the coated conductor tapes or their superconducting films, respectively, are superconductively connected along their extension direction (z).
- a local defect in one of the coated conductor tapes may be bypassed locally; the coated conductor tape having the defect may still contribute to the current carrying capacity of the superconductive structure at a distance (in z) from its defect (where, in turn, possibly another coated conductor tape may have a local defect to be bypassed). Accordingly, the current carrying capacity of the superconducting structure is used more efficiently.
- the superconductive connection between two coated conductor tapes along the extension direction z may be continuous, what allows a redistribution of currents everywhere along the extension direction, or intermittent, what allows a redistribution at every connection area located along the extension direction.
- Coated conductor tapes connected intermittently along the extension direction are not only connected at the ends of the coated conductor tapes, but also several times between the ends, typically in a periodic way, and preferably over at least one third of the total length (in z) of the superconducting structure.
- a coated conductor tape of the inventive superconductive structure which provides a superconductive current path for a part of the current to be conducted (“partial superconductive current path”), is directly superconductively connected to at least one—and typically two or three—further coated conductor tapes, wherein the superconducting film sides of said coated conductor tape and said at least one further coated conductor tape face each other.
- the opposing superconducting films typically touch each other or are separated only by a thin solder layer, in particular of a noble metal or noble metal alloy (preferably containing gold and/or silver), or by a combination of a thin solder layer, in particular of a noble metal or noble metal alloy (preferably containing gold and/or silver) and thin capping layers (typically of copper) of the coated conductor tapes, so that—if at all—only a negligible electric resistance is introduced, and superconductivity is maintained across the connection, i.e. a redistribution of currents between the opposing superconducting films does not result in a quench.
- a solder layer may contain tin and/or may be free of noble metals, if desired. With a total thickness of the solder layer and possible capping layers of 100 ⁇ m or less at the connection, preferably 30 ⁇ m or less, a negligible ohmic resistance can normally be achieved.
- coated conductor tapes facing each other with their superconducting film sides typically only partially overlap with respect to a direction (y, y′) in parallel to the substrate planes and perpendicular to the extension direction (z), in order to enlarge the structure in y, y′-direction.
- coated conductor tapes contributing to an enlargement of the superconducting structure in direction x, x′ basically perpendicular to the substrate planes may also have a complete overlap in y, y′-direction (such as Y-elements, see below).
- each coated conductor tape providing one of the parallel partial current paths is directly superconductively connected to every other such coated conductor tape; an indirect connection (i.e. via one or more other coated conductor tapes) is sufficient for the redistribution of the current among these coated conductor tapes.
- the coated conductor tapes may be linearly connected (in the xy cross-sectional plane), so that each coated conductor tape has only two direct connections at maximum; when using also coated conductor tapes connected to three or even more coated conductor tapes, a true 2-dimension network in cross-section perpendicular to z may be realized.
- coated conductor tapes each have a length (in z direction) which is much larger, typically at least ten times larger, than their width (in y, y′-direction); the width in turn is much larger, typically at least ten times larger, than their height (in x, x′ direction).
- the coated conductor tapes are typically stacked (arranged one above the other) in a direction (x, x′) basically perpendicular the substrate planes (or tape surfaces, respectively) of the coated conductor tapes.
- a superconducting structure includes typically at least four coated conductor tapes, and preferably more than ten coated conductor tapes providing superconducting partial current paths.
- the superconducting films preferably include HTS material, such as YBCO.
- Typical and preferred applications for the inventive superconducting structures are superconducting cables. Note that a superconducting structure does not need to run straight in an extension direction z, but may be bent or curved, in particular in cable applications.
- the coated conductor tapes form a labyrinth structure comprising at least three levels of coated conductor tapes
- coated conductor tapes of each level are superconductively connected in a linear sequence in a direction (y, y′) basically parallel to the substrate planes and perpendicular to the extension direction (z),
- coated conductor tapes of each two levels neighboring in a direction (x, x′) basically perpendicular to the substrate planes of the coated conductor tapes are superconductingly connected to each other via at least one of their coated conductor tapes each, in particular via a lateral coated conductor tape of the level, thus allowing a balancing of currents within the superconducting structure in said direction (x, x′) basically transverse to the respective substrate planes of the coated conductor tapes.
- a balancing of currents in parallel to the substrate planes (across the width of the coated conductors)
- a balancing of currents (or a free distribution of currents) in a direction (x, x′) basically perpendicular to the substrate planes is provided; typically, the coated conductors build a stack in the x, x′-direction for this purpose.
- the invention allows a balancing of currents in said direction (x, x′) transverse to the respective substrate planes typically within at least four, preferably at least ten coated conductor tapes (or their respective levels) arranged next to each other in said direction (x, x′).
- the superconductive connection between levels is done via lateral coated conductor tapes (which are at the side ends of a respective level with respect to the y, y′ direction), with one end connecting upwards and one end connecting downwards in x, x′ direction (thus allowing a “back and forth” redistribution of currents in y direction within the labyrinth structure).
- the total critical current of a labyrinth structure exceeds the sum of the particular critical currents of the parallel coated conductor tapes taken along (comprised). This effect is not fully understood by the inventors, because the critical current gain is more than what should follow from the effect of bypassing of local defects (i.e. the effect of mutual shunting). Typically, the gain reaches 30% to 50%, what is at least two times higher than one may expect from current bypassing.
- Another effect that may be achieved in the labyrinth structure is a suppressing of coated conductor tape damage in the course of a quench event.
- “Wider” distributed current in the labyrinth structure creates smoothed overheated spots (“hot spots”) with a temperature which is typically below the damage threshold.
- free space in the superconducting structure not filled with coated conductor tapes is partially or completely filled with metal or a dielectric material.
- Such fillings may generally mechanically adjust, in particular stabilize, the structure.
- the shunt protection may be improved.
- a cooling agent in particular wherein the cooling agent exhibits a mass flow in the extension direction.
- the coated conductor tapes may be efficiently cooled, and the free space is advantageously used.
- Typical cooling agents to be used are liquefied gases, in particular LN2 and LHe. In the direction of the extension direction z, a laminar flow of the cooling agent is easy to establish.
- the coated conductor tapes are slightly curved in a cross-section perpendicular to the extension direction (z). In this way the structure can be adjusted to external needs, such as the desired installation path of a cable made from the structure. Note that by bending around the extension direction z over some distance in z, a structure of geometrically parallel coated conductor tapes may be bent over the short side in a desired direction which represented a non-accessible direction (such as the long side of the coated conductor tapes) before.
- the coated conductor tapes are periodically arranged in a direction (x, x′) basically perpendicular to the substrate planes.
- a periodic arrangement By means of a periodic arrangement, a simple structure which can be extended as needed is provided.
- the superconducting structure may (independent of a periodicity in x, x′-direction) also be periodic in y, y′-direction, such as with two or more, preferably five or more repetition units.
- a further advantageous embodiment provides that at least some of the coated conductor tapes each are bent such that a first part of the width of the coated conductor tape is offset with respect to a second part of the coated conductor tape in a direction (x, x′) basically perpendicular to the substrate plane.
- coated conductor tapes are stacked in a direction (x, x′) basically perpendicular to the substrate planes, thus forming a stack.
- a particularly compact superconducting structure can be achieved, accessing the x, x′-dimension.
- the electric current can be distributed differently in x, x′-direction within the stack along the extension direction z.
- a stack typically comprises at least four, preferably at least ten coated conductor tapes stacked in x, x′-direction.
- the stack is typically periodic in x, x′-direction. Further note that the stack may include several coated conductor tapes per x, x′-direction level (tape layer), typically wherein said several coated conductor tapes partially overlap in y, y′-direction.
- At least some coated conductor tapes within the stack each are superconductively connected at least to a first further coated conductor tape and a second further coated conductor tape
- first further coated conductor tape directly or indirectly establishes a superconducting connection of the coated conductor tape to coated conductor tapes above said coated conductor tape within the stack
- the second coated conductor tape directly or indirectly establishes a superconducting connection to coated conductor tapes below said coated conductor tape within the stack.
- the coated conductor tapes are stacked in a closed ring shaped fashion, thus forming a ring-shaped stack, with the circumferential direction (x′) of the ring-shaped stack basically perpendicular to the substrate planes.
- the coated conductor tapes are arranged one above another, with a slight tilt relative to each other; the next neighbors of coated conductor tapes in x′-direction typically do not abut flatly here, and/or at least a part are even spaced apart.
- the electric current may also balance in circumferential direction.
- the ring-shaped stack includes a core free from coated conductor tapes.
- the density of coated conductor tapes along the circumference of the ring-shaped stack is constant, and the ring-shaped stack is circular. Then circular magnetic fields of high quality are achievable, although tape type coated conductors are used for their generation.
- the superconducting structure includes spacers filling spaces in at least one non-dense section of the superconducting structure in which less coated conductor tapes are stacked in the direction (x; x′) basically perpendicular to the substrate planes than in a dense section in which the coated conductor tapes neighboring in the direction (x, x′) basically perpendicular to the substrate planes abut each other.
- spacers thickness differences between dense and non-dense sections in stacks can be leveled. This increases the stability of the superconducting structure.
- the spacers comprise coated conductor tape pieces, which are not superconductively connected to another coated conductor tape, and which are bent inwards the superconducting structure. If the structure provides no dedicated edge tapes, the coated conductor tapes at the edges (which are often not included in any current carrying function) may be bent in so they can still take over a spacer function. The double material in the bent region fills in the non-dense sections with the proper height.
- the superconducting structure comprises at least one Y-element, each with two coated conductor tapes facing each other with their respective superconducting film sides, wherein said two coated conductor tapes are superconductingly connected along the extension direction (z) continuously or intermittently in a connection region, and wherein said two coated conductor tapes are spaced apart in a direction (x, x′) basically perpendicular to the substrate planes in a transfer region on one side of the connection region.
- the superconducting structure comprises a plurality of Y-elements, which are directly or indirectly interconnected.
- the two coated conductor tapes may be superconductively connected to a further coated conductor tape each.
- One or both of the further coated conductor tapes may be in turn part of Y-elements.
- the two coated conductor tapes of the Y-element extend differently far within the transfer region in a direction (y, y′) basically parallel to the substrate planes and perpendicular to the extension direction (z).
- the Y-element comprises an additional transfer region in which the two coated conductor tapes are spaced apart in a direction (x, x′) basically perpendicular to the substrate planes, wherein the transfer region and the additional transfer region are separated by the connection region.
- Such double Y-elements may in particular bridge between lateral Y-elements (and further double Y-elements and/or S-elements, see below).
- Double Y-elements allow a true 2-dimensional connection network in cross-section perpendicular to the z direction. More specifically, with the double Y-elements, honeycomb-like structures may be built, providing a particularly safe and flexible connection network.
- said two coated conductor tapes of the Y-element in the transfer region comprise protrusions and recesses with respect to a direction (y, y′) basically parallel to the substrate planes and perpendicular to the extension direction (z), alternating in the extension direction (z), and that the protrusion and recess patterns of said two coated conductor tapes are offset in the extension direction (z). This avoids thickness differences within the superconducting structure. Due to the offset, protrusions of one of the two coated conductor tapes coincide (in z) with recesses of the other of the two coated conductor tapes.
- the superconducting structure comprises at least one S-element, with two coated conductor tapes facing each other with their respective superconducting film sides, wherein said two coated conductor tapes are superconductively connected in a connection region, and wherein the two coated conductor tapes extend beyond the connection region on opposing sides in a direction (y, y′) basically in parallel with the substrate planes but basically perpendicular to the extension direction (z).
- a superconducting structure may be extended in y, y′-direction by simple means.
- S-elements may in particular bridge between lateral Y-elements (and further S-elements and/or double-Y-elements).
- each two coated conductor tapes superconductively connected face each other with their superconducting film sides, and the superconducting films are electrically connected
- FIG. 1 a schematic, perspective and partially cross-sectional view of an embodiment of an inventive superconducting structure, with coated conductor tapes connected in a chain-like fashion in a direction (y) basically in parallel to the substrate planes and perpendicular to an extension direction (z) of the coated conductor tapes;
- FIG. 2 a schematic, perspective and partially cross-sectional view of an embodiment of an inventive superconducting structure of labyrinth type, based on Y-elements stacked in a direction (x) basically perpendicular to the substrate planes of the superconductive structure, with a non-dense stack;
- FIG. 3 a schematic cross-section of an embodiment of an inventive superconductive structure similar to FIG. 2 , with the stack comprising a dense section and two non-dense sections;
- FIG. 4 a a schematic cross-section of an embodiment of an inventive superconductive structure similar to FIG. 3 , but with spacers filling spaces in the non-dense sections;
- FIG. 4 b a schematic cross-section of an embodiment of an inventive superconductive structure similar to FIG. 4 a , wherein the spacers are inwardly bent coated conductor tape pieces;
- FIG. 5 a a schematic cross-section of an embodiment of an inventive superconductive structure similar to FIG. 3 , with a dielectric filling free space of the structure;
- FIG. 5 b a schematic cross-section of an embodiment of an inventive superconductive structure similar to FIG. 3 , wherein a cooling agent, flowing within a tube and through the structure, cools the structure;
- FIG. 6 a schematic cross-section of an embodiment of an inventive superconductive structure similar to FIG. 3 , wherein the coated conductor tapes of each Y-element extend differently far into a transfer region;
- FIG. 7 a - 7 b an illustration of an embodiment of an inventive superconductive structure similar to FIG. 3 , wherein the coated conductor tapes have protrusions and recesses in a transfer region, in a schematic cross-section ( FIG. 7 a ) and a schematic top view ( FIG. 7 b );
- FIG. 8 a schematic cross-section of an embodiment of an inventive superconductive structure of labyrinth type, based on Y-elements and double Y-elements in a non-dense stack;
- FIG. 9 a schematic cross-section of an embodiment of an inventive superconductive structure, based on interconnected Y-elements and S-elements;
- FIG. 10 a schematic cross-sectional view of an embodiment of an inventive superconductive structure of labyrinth type, based on Y-elements stacked in a closed ring-type fashion;
- FIG. 11 a schematic cross-section of a Y-element for use with the invention.
- FIG. 1 illustrates an embodiment of an inventive superconducting structure 1 .
- the structure 1 (and the superconducting structures 1 introduced in the following figures) is supposed to carry an electric current I superconductively in an extension direction z.
- the structure 1 comprises here five coated conductor tapes 2 , each with a substrate 3 and a superconducting film 4 on (only) one of its sides, well visible in the cross-section in the front part of the figure.
- the substrate 3 may be of a flexible steel type
- the superconducting film 4 may comprise YBCO material.
- one or more buffer layers may be deposited between the substrate 3 and the superconducting film 4 , and further auxiliary layers known in the art may be provided, if needed.
- the coated conductor tapes 2 face each other with their superconducting films 4 .
- each coated conductor tape 2 overlaps with a part of its width W over its full length L with two other coated conductor tapes 2 , with an offset (i.e. being shifted) in a direction y basically in parallel with the substrate planes and perpendicular to the extension direction z.
- the overlap region OR which extends in z direction over the complete length L
- the overlapping coated conductor tapes 2 are continuously superconductively connected.
- electric current I flowing superconductingly in z direction may be redistributed in y direction between all superconducting films 4 of the five coated conductor tapes 2 ; the coated conductor tape 2 (or their superconducting films 4 , respectively) represent parallel current paths.
- FIG. 2 shows an embodiment of an inventive superconducting structure 1 based on Y-elements 5 a - 5 d .
- the shown structure 1 here comprises four interconnected Y-elements 5 a - 5 d , but may be extended periodically as desired in x direction.
- a Y-element 5 a comprises two coated conductor tapes (also referred to as coated conductors) 2 a , 2 b , each with a substrate 3 and a superconducting film 4 , with the superconducting film sides facing each other.
- the superconducting films 4 of the coated conductor tapes 2 a , 2 b are (here) continuously superconductively connected over their full length L along the extension direction z.
- the coated conductor tapes 2 a , 2 b are spaced apart from each other, such that a mouth-like opening 6 results in cross-section (Note that in the figures, the dimensions in x direction, including the height H of the coated conductor tapes, is shown enlarged as compared to the dimensions in y direction, including width W, for easier comprehension).
- a coated conductor tape see e.g. coated conductor tape 2 b , in the transfer region TR (or in the mouth like opening 6 , respectively) may be superconductively connected (here continuously over the full length L of the coated conductors) to another coated conductor tape, see e.g. coated conductor tape 2 c of a further Y-element 5 c . Accordingly, electric current I may be transferred between the Y-elements 5 a , 5 c in the transfer region TR.
- Y-element 5 c is in turn superconductively connected to Y-element 5 b , and the latter to Y-element 5 d , so free distribution of the electric current I flowing in z direction (or a balancing of currents, respectively) within the parallel coated conductor tapes may occur along the chain of electrically interconnected Y-elements 5 a - 5 c - 5 b - 5 d , and thus also in a direction x basically perpendicular to the substrate planes which are basically parallel to the yz plane here.
- connecting regions CR and the transfer regions TR typically have about the same width in y direction. It is also possible to choose the widths of said regions differently, in particular with the transfer regions TR wider than the connection regions CR in y direction, in order to mechanically stabilize a center of the superconducting structure 1 .
- the superconducting structure 1 of FIG. 2 is of a labyrinth type, comprising coated conductor tapes in three levels, namely Lv 1 (with tapes 2 b , 2 c ), further Lv 2 (with tapes 2 p , 2 d ), and further Lv 3 (with tapes 2 q , 2 r ).
- Lv 1 with tapes 2 b , 2 c
- Lv 2 with tapes 2 p , 2 d
- Lv 3 with tapes 2 q , 2 r .
- Lv 2 is connected on the right end via its coated conductor tape 2 p to coated conductor tape 2 c of Lv 1 , and on the left end via its coated conductor tape 2 d to coated conductor tape 2 q of Lv 3 .
- the connections between the levels Lv 1 -Lv 3 allow a current redistribution in x direction between the levels, accordingly.
- coated conductor tapes see for example coated conductor tape 2 b , are somewhat bent, so that a first part P 1 of the coated conductor tape 2 b , here at the connection region CR, is offset (shifted) in x direction with respect to a second part P 2 of the coated conductor tape 2 b , here in the transfer region TR.
- the x direction becomes accessible for the superconducting structure 1 , i.e. a superconducting connection may be established between coated conductors arranged one above the other in x direction (“stacked in x direction”).
- coated conductor tapes 2 d and 2 b are connected via Y-element 5 c by means of its two bent coated conductor tapes.
- coated conductor tapes 2 b , 2 d neighboring in x direction are spaced apart by a spacing SP.
- free space 7 a within the structure 1 (not filled with coated conductors) is not minimized here.
- This gives the superconducting structure 1 although stacked, a good flexibility, in particular when bending the structure 1 upwards or downwards in x direction with e.g. its front end (“over the short side”).
- a support frame may be used to establish and define said spacing SP (not shown).
- a minimum (non-zero) spacing SP is provided between at least some of the Y-elements 5 a - 5 d (or, more generally, at least some of the coated conductor tapes) of a superconducting structure 1 neighboring in a stack in x direction, the stack can be called non-dense.
- FIG. 3 shows, now in cross-section only (for simplification, what also applies to the subsequent figures), a superconducting structure 1 similar to the one of FIG. 2 , but with a dense section DS in the center of the structure 1 .
- the dense section DS the neighboring Y-elements 5 (or the neighboring coated conductor tapes 2 ) are all flatly abutting each other, so no minimum spacing is kept. By this measure, free space 7 a in the structure 1 is minimized here. This gives a very compact design.
- non-dense sections ND exhibit only half the number coated conductor tapes as compared to the dense section DS, what may lead to an unintentionally strong (and possibly damaging) bending, in particular when a large number of coated conductor tapes 2 is stacked in x direction.
- the design of the superconducting structure 1 is significantly more compact than shown in the schematic FIG. 3 (and the further figures) because of a low aspect ratio, i.e. ratio of the thickness (height) of a coated conductor to its width; the aspect ratio yields typically from 1:20 to 1:200. Due to this, the volume content of a dense section DS may significantly dominate the volume content of non-dense sections ND as well as of sections located in between a dense section DS and a non-dense section ND.
- spacers 8 may be inserted into the spaces 7 , compare FIG. 4 a .
- the spacers 8 which are typically stripes (extending in z direction), may be of an arbitrary solid material; it may be useful to use a metal, in particular a well conducting metal such a copper, in order to provide a shunt resistance.
- the spacers 8 partially fill the free space 7 a of the structure 1 .
- coated conductor tape material may be used for filling purposes.
- coated conductor tape pieces 16 , 17 bent inwardly towards the superconducting structure 1 may be used as spacers.
- the bent coated conductor tape pieces 16 , 17 have exactly the correct height in x-direction to fill the empty spaces 7 in the non-dense sections ND. Note that each space 7 may be filled simply with one coated conductor tape piece 16 , or with the ends of two coated conductor tape pieces 17 (then each coated conductor tape piece 17 may contribute to the filling of two spaces 7 ).
- the coated conductor tape pieces 16 , 17 with a spacer function are preferably not superconductively connected to the coated conductor tapes 2 carrying the superconducting electric current within the superconductive structure 1 .
- FIG. 5 a illustrates an embodiment of an inventive superconducting structure 1 comparable to the one shown in FIG. 3 , but with a dielectric material (e.g. of epoxy type, marked lightly dotted) 18 filling the free space of the structure 1 .
- the dielectric (electrically insulating) material 18 is preferably applied in a liquid form, so a complete (or almost complete) filling of the free space may be achieved, and hardened later on, so a mechanical stabilization can be achieved, comparable to or even better than the one achieved with spacers.
- FIG. 5 b shows an embodiment of an inventive superconducting structure 1 comparable to the structure shown in FIG. 3 again; here the structure 1 is put into a tubing 20 , in which a cooling agent 19 (marked with a wavy pattern) flows in z direction (perpendicular to the plane of the cross-sectional drawing).
- the cooling agent 19 e.g. liquid helium (LHe)
- LHe liquid helium
- a temperature below the critical temperature Tc of the superconducting material of the coating conductor tapes 2 may be kept easily.
- the coated conductor tapes 2 of a Y-element 5 reach differently far into the transfer region TR, compare FIG. 6 .
- the top coated conductor tape 2 e of each Y-element 5 extends less far into the transfer region TR as compared to the bottom coated conductor tapes 2 f , and the short top coated conductor tapes 2 e of opposing Y-elements 5 do not overlap.
- the number of coated conductor tapes stacked in every part of the transfer region TR is only one and a half times the number of coated conductor tapes in the connection regions CR within the superconducting structure 1 (as compared to two times, in the embodiment of FIG. 3 ).
- FIG. 7 a in cross-section
- FIG. 7 b in top view
- the coated conductor tapes 2 g - 2 k have protrusions 9 and recesses 10 , reaching into and being retracted from the transfer region TR, and alternating in z-direction, here in a wave-like manner.
- the protrusions 9 and recesses 10 lead to a uniform number of coated conductor tapes stacked in x-direction all over the superconducting structure 1 , namely both within the connecting regions CR and the transfer region TR.
- FIG. 7 b (and in the overlaps in FIG. 7 a ), with the full lines, the contours of the top coated conductor tape 2 g of Y-element 5 e and the bottom coated conductor tape 2 k of Y-element 5 f are shown. With the dashed lines, the contours of the bottom coated conductor tape 2 h of Y-element 5 e and the top coated conductor tape 2 i of Y-element 5 f are shown (note that the Y-elements 5 e on the left of the superconducting structure 1 are all identical, and the Y-elements 5 f on the right of the superconductive structure 1 are all identical, too). For better understanding, the Y-elements 5 e , 5 f are shown pulled apart in y direction in FIG. 7 b.
- the bottom coated conductor tape 2 h has a recess 10 .
- the top coated conductor tape 2 i has a recess 10
- the bottom coated conductor tape 2 k has a protrusion 9 . Accordingly, the left top coated conductor tape 2 g and the right bottom coated conductor tape 2 k can be superconductively connected at the protrusion overlap (hatched areas in FIG. 7 b ), whereas the left bottom coated conductor tape 2 h and the right top coated conductor tape 2 i do not overlap here.
- the top coated conductor tape 2 g has a recess 10 .
- the bottom coated conductor tape 2 k has a recess 10
- the top coated conductor tape 2 i has a protrusion 9 . Accordingly, the left bottom coated conductor tape 2 h and the right top coated conductor tape 2 i can be superconductively connected at the protrusion overlap (dotted areas in FIG. 7 b ), whereas the left top coated conductor 2 g and the right bottom coated conductor 2 k do not overlap here.
- any two coated conductor tapes connected via protrusion overlap have, in z direction, an overlap at about half of the total length L of the superconducting structure 1 .
- FIG. 8 shows an embodiment of an extended superconducting structure 1 in accordance with the invention.
- the structure 1 comprises on its outer (edge) sides Y-elements 5 , which are interconnected via double Y-elements 11 .
- a double Y-element 11 comprises two coated conductor tapes 2 l , 2 m , facing each other with their superconducting film sides (see substrates 3 and superconducting films 4 ) which are superconductively connected at a central connection region CR, and spaced apart at mouth-like openings 6 in a transfer region TR and an additional transfer region ATR provided at the two sides of the connection region CR in y direction.
- ATR coated conductor tapes, in particular of Y-elements 5 and double Y-elements 11 , may be superconductively connected.
- superconducting structures 1 with honeycomb like patterns in cross-section may be built (compare the approximately hexagonally shaped spaces 7 a ).
- Such a pattern provides multiple alternative currents paths (in the xy plane) for a superconducting current between any two coated conductor tapes in the superconducting structure 1 .
- This increases the defect tolerance of the superconductive structure 1 .
- the honey comb like pattern is particularly flexible. High mechanical flexibility of the inventive superconductive structure 1 is particularly appreciated for superconducting cables.
- the inventive structure 1 of FIG. 8 is also of labyrinth type, (here) with five levels Lv 1 -Lv 5 , each with (here) four coated conductor tapes connected in linear sequence.
- Each two levels neighboring in x direction e.g. levels Lv 1 and Lv 2
- Lv 1 and Lv 2 are connected to each other multiple times here, namely both via a lateral Y-element 5 (on the right in FIG. 8 for Lv 1 and Lv 2 ) and via a double Y-element 11 .
- FIG. 9 illustrates an embodiment of a superconducting structure 1 using a mixture of Y-elements 5 and S-elements 12 in an arbitrary design.
- An S-element 12 comprises two coated conductor tapes 2 n , 2 o , facing each other with their superconducting film sides (see substrates 3 and superconducting films 4 ) and superconductively connected (here) continuously in a connection region CR where the two coated conductor tapes 2 n , 2 o overlap. Both coated conductor tapes 2 n , 2 o extend (in y direction) beyond the connecting region CR on opposing sides (right and left in the figure); these parts may be used for connecting to a further coated conductor tape (e.g. as part of a Y-element 5 ).
- An S-element 12 may be used to superconductively connect two Y-elements 5 , for example, as shown in FIG. 8 .
- a superconducting structure 1 may also include singe coated conductor tapes 2 not belonging to Y-elements, double Y-elements or S-elements.
- FIG. 10 illustrates another embodiment of an inventive superconductive structure 1 .
- This superconducting structure 1 is based on Y-elements 5 g , 5 h here, which build a ring-shaped stack 13 , providing a closed superconducting current path around a core 15 .
- Said core 15 may be separated from the superconducting structure 1 by means of a tube 14 .
- the Y-elements 5 g , 5 h are superconductively connected via superconducting films 4 (see thick black lines) on substrates 3 of coated conductor tapes 2 facing each other with their superconducting film sides, similar to the embodiment shown in FIG. 2 .
- the radially inner Y-elements 5 h are slightly differently bent as compared to the radially outer Y-elements 5 g , here with the Y-elements 5 h opening out with the coated conductor tape ends reaching radially outward, and the Y-elements 5 g with parallel coated conductor tape ends reaching radially inward. Neighboring Y-elements 5 h , 5 g are slightly rotated with respect to each other.
- the Y-elements 5 g , 5 h are evenly distributed around the circumference of the superconducting structure 1 , and together have a basically circular shape.
- the Y-elements 5 g , 5 h or their coated conductor tapes, respectively, are stacked in circumferential direction x′, which is perpendicular to the respective local substrate planes; the substrate planes are basically in parallel to the local y′z plane, with direction y′ being the local radial direction here (which is in parallel with the local substrate planes, and perpendicular to the extension direction z).
- the superconducting structure 1 provides a deeply distributed magnetic field along the radius. This field causes a more uniform interaction with entire structure 1 (compared e.g. to a typical conventional cable configuration), and as a result should homogenize a quench across entire radial depth.
- spaces within the ring-shaped (non-dense) stack 13 are not filled with spacers, so a maximum flexibility of the structure 1 is provided.
- This superconducting structure 1 is particularly suited for use in a superconducting cable.
- the field-free core 15 can be used for a signal transmission save from external disturbances.
- a ring-shaped stack 13 in accordance with the invention, need not be based on Y-elements only, but may include other elements, such as double Y-elements or S-elements, or coated conductor tapes not belonging to particular elements, too.
- FIG. 11 details an example of a Y-element 5 for use within an inventive superconducting structure.
- the Y-element 5 comprises two coated conductor tapes 2 a , 2 b , superconductively connected at a connection region CR.
- the coated conductor tapes 2 a , 2 b are surrounded by a capping layer 17 of copper each, and at the connection region CR, the coated conductor tapes 2 a , 2 b are connected via a solder layer 16 , for example containing silver and/or tin. Electric current running through the superconducting films 4 of the tapes 2 a , 2 b may redistribute between the films 4 across the capping layers 17 and the solder layer 16 .
- the total thickness D int of any intermediate layers 16 , 17 is in general 100 ⁇ m or less, preferably 30 ⁇ m or less, in order to keep the ohmic resistance sufficiently low, e.g. at the level below 30 nOhms*cm 2 , preferably below 3 nOhms*cm 2 .
- the total contact area of two coated conductor tapes is at least 100 cm 2 , preferably at least 1000 cm 2 .
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Abstract
Description
thus allowing a balancing of currents within the superconducting structure in said direction (x, x′) basically transverse to the respective substrate planes of the coated conductor tapes.
-
- by touching each other directly, or
- across a solder layer, in particular of a noble metal or a noble metal alloy, or
- across capping layers, in particular copper capping layers, of the coated conductor tapes and a solder layer, in particular of a noble metal or a noble metal alloy. While a direct touching of the superconducting films may result in a highest quality contact, intermediate solder and/or capping layers are often used since they are easier to handle during production, in particular as far as durability of the contact is concerned. In practice, some negligible (i.e. very low) ohmic resistance is almost inevitably introduced at any connection of each two opposing coated conductor tapes (in particular if one or more intermediate layers are used), but due to the large contact area (along the length of the parallel tapes), this ohmic resistance does not impair the use of the inventive superconducting structure as a whole. Accordingly, such quasi-superconductively connected coated conductor tapes are still considered to qualify as a superconducting connection in accordance with the invention.
Claims (32)
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
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EP20120154480 EP2626868B1 (en) | 2012-02-08 | 2012-02-08 | Superconducting structure comprising coated conductor tapes, in particular stapled perpendicularly to their substrate planes |
EP12154480 | 2012-02-08 | ||
EP12154480.3 | 2012-02-08 |
Publications (2)
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US20130203604A1 US20130203604A1 (en) | 2013-08-08 |
US9008741B2 true US9008741B2 (en) | 2015-04-14 |
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US13/760,110 Expired - Fee Related US9008741B2 (en) | 2012-02-08 | 2013-02-06 | Superconducting structure comprising coated conductor tapes, in particular stapled perpendicularly to their substrate planes |
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GB201515978D0 (en) | 2015-09-09 | 2015-10-21 | Tokamak Energy Ltd | HTS magnet sections |
DE102015219956A1 (en) * | 2015-10-14 | 2017-04-20 | Bruker Hts Gmbh | Superconductor structure for connecting strip conductors, in particular with a wavy or serrated seam |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0545608A2 (en) | 1991-12-02 | 1993-06-09 | General Electric Company | Superconducting joint for oxide superconductor tape |
US20050173679A1 (en) * | 2002-02-21 | 2005-08-11 | Mannhart Jochen D. | Superconductors and methods for making such superconductors |
US20080210454A1 (en) * | 2004-03-31 | 2008-09-04 | Michael Fee | Composite Superconductor Cable Produced by Transposing Planar Subconductors |
US7774035B2 (en) | 2003-06-27 | 2010-08-10 | Superpower, Inc. | Superconducting articles having dual sided structures |
US20120309631A1 (en) | 2009-08-10 | 2012-12-06 | Bruker Hts Gmbh | High temperature superconductor current lead for connecting a superconducting load system to a current feed point |
-
2012
- 2012-02-08 EP EP20120154480 patent/EP2626868B1/en not_active Not-in-force
-
2013
- 2013-02-06 US US13/760,110 patent/US9008741B2/en not_active Expired - Fee Related
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0545608A2 (en) | 1991-12-02 | 1993-06-09 | General Electric Company | Superconducting joint for oxide superconductor tape |
US20050173679A1 (en) * | 2002-02-21 | 2005-08-11 | Mannhart Jochen D. | Superconductors and methods for making such superconductors |
US7774035B2 (en) | 2003-06-27 | 2010-08-10 | Superpower, Inc. | Superconducting articles having dual sided structures |
US20080210454A1 (en) * | 2004-03-31 | 2008-09-04 | Michael Fee | Composite Superconductor Cable Produced by Transposing Planar Subconductors |
US20120309631A1 (en) | 2009-08-10 | 2012-12-06 | Bruker Hts Gmbh | High temperature superconductor current lead for connecting a superconducting load system to a current feed point |
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EP2626868A1 (en) | 2013-08-14 |
US20130203604A1 (en) | 2013-08-08 |
EP2626868B1 (en) | 2014-04-02 |
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